Table 3: of results with a smaller disc ( $R=10^{14}~{\rm cm}$ ), else as for Table 1. F₀ is the signed flux through the disc plane in $r\le 1$ (corresponding to 10¹⁴ cm) and $B_{\rm ext}^{(14)}$ is the dimensionless strength of the external field, but now measured in the units of $k^{1/2}B_{\rm eq}$ at that radius.
$B_{\rm ext}^{(14)}$ $E_{\rm t}\times10^{-4}$ $E_{\rm d}\times10^{-4}$ $s\times10^6$ F₀

0.0 7.5 3.7 1.0 0.28

0.01 7.9 3.9 1.1 0.33

0.10 $13\phantom{0}\phantom{0}$ 5.6 6.9 0.79

1.0 $240\phantom{0}\phantom{0}\phantom{0}\phantom{0}$ $63\phantom{0}\phantom{0}$ $33\phantom{0}\phantom{0}$ 5.84

10.0 $2.1\times10^4$ $5.1\times10^3$ $39\phantom{0}\phantom{0}$ 56.4

**Table 3:** of results with a smaller disc ( $R=10^{14}~{\rm cm}$ ), else as for Table 1. F₀ is the signed flux through the disc plane in $r\le 1$ (corresponding to 10¹⁴ cm) and $B_{\rm ext}^{(14)}$ is the dimensionless strength of the external field, but now measured in the units of $k^{1/2}B_{\rm eq}$ at that radius.
$B_{\rm ext}^{(14)}$	$E_{\rm t}\times10^{-4}$	$E_{\rm d}\times10^{-4}$	$s\times10^6$	F₀
0.0	7.5	3.7	1.0	0.28
0.01	7.9	3.9	1.1	0.33
0.10	$13\phantom{0}\phantom{0}$	5.6	6.9	0.79
1.0	$240\phantom{0}\phantom{0}\phantom{0}\phantom{0}$	$63\phantom{0}\phantom{0}$	$33\phantom{0}\phantom{0}$	5.84
10.0	$2.1\times10^4$	$5.1\times10^3$	$39\phantom{0}\phantom{0}$	56.4

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